ライフサイエンスコーパス: electronic transition

1 he subscript indicates the wavelength of the electronic transition).

2 data without considering the effects of the electronic transition.

3 ute polarizability is allowed to change with electronic transition.

4 n about the degree of charge transfer in the electronic transition.

5 ystem as well as vibrational coupling to the electronic transition.

6 the lanthanide signal and assign underlying electronic transitions.

7 h absorption spectra reveals four low-energy electronic transitions.

8 arge-transfer) formulation of donor/acceptor electronic transitions.

9 erved when activated vibrations overlap with electronic transitions.

10 energy dependence, which could be caused by electronic transitions.

11 otoexcited wave function due to nonadiabatic electronic transitions.

12 ed phosphors involves multiple mechanisms of electronic transitions.

13 edium via their rotational, infrared, and/or electronic transitions.

14 elopment of the low- and high-spin intersite electronic transitions.

15 rs the intensity borrowing from spin-allowed electronic transitions.

16 vided further insight into the nature of the electronic transitions.

17 in a systematic blue shift in the low-energy electronic transitions (7, 523 nm; 8, 505 nm; 9, 445 nm

18 vealed well-resolved first- and second-order electronic transitions accompanied by prominent sideband

19 mplete and direct microscopic picture of the electronic transition across the YBCO/LCMO interfaces, w

20 The electronic transition affords modulation of the opto-ele

21 The convergence of these electronic transitions agrees with theoretical treatment

22 nd that during both heating and cooling, the electronic transition always precedes the structural Pei

23 luorescent properties, and molecular orbital electronic transition analysis establish that its fluore

24 For complex III, the slightly red-shifted electronic transition and the stoichiometry are most con

25 oseconds, as well as associated photoinduced electronic transitions and charge transfer processes.

26 However, the low-energy electronic transitions and resonance Raman features attr

27 molecule-like properties, including discrete electronic transitions and strong fluorescence.

28 The blue shifts in the electronic transitions and the bisignate shape of the ci

29 ,0 band is composed of two nearly degenerate electronic transitions and the split is due to the asymm

30 ) excited within the peptide bond pi --> pi* electronic transitions and within the aromatic amino aci

31 ured and revealed a strong dependence of the electronic transitions and, therefore, the colors upon t

32 ) and of valence-to-core (Kss(2,5) emission) electronic transitions, and of Kalpha RIXS data, which w

33 mission wavelengths, to suppress undesirable electronic transitions, and to sensitize absorption of l

34 even in isotropic samples when well-defined electronic transitions are excited.

35 ot one but two nearly orientation-degenerate electronic transitions are required to explain the 340-5

36 ly at 440 gigapascals might be related to an electronic transition associated with pressure-induced i

37 empts to explain this coupled structural and electronic transition begin with two alternative startin

38 de were observed with strong, characteristic electronic transitions between 400 and 600 nm.

39 le conical intersection is implicated in the electronic transition but the excited state reaction lea

40 n PcoA, binds one Cu(II) and exhibits a weak electronic transition characteristic of a type II copper

41 e observe spectral bleaching of the nanotube electronic transitions consistent with an electron-trans

42 ich is converted to vibrational energy after electronic transitions could lead to athermal hot ground

43 temperature dependence of the MBCT and MMCT electronic transitions defines the mixed valence complex

44 taking into account the distribution of the electronic transition densities in the dots and using th

45 due to resonance with new optically allowed electronic transitions, determined by the relative orien

46 In the dyad, the electronic transition dipole moment of the electron dono

47 obtain information on the directions of the electronic transition dipole moments ((-->)m) of the chr

48 ive angle and separation between interacting electronic transition dipole moments and thus provide a

49 ically determined the relative angle between electronic transition dipole moments of its chlorophyll

50 vestigation of the dependence of the allowed electronic transition energies (electronic origins) on c

51 c experiments have permitted us to determine electronic transition energies and polarizations, as wel

52 H) MCD spectroscopies were used to determine electronic transition energies and to obtain an estimate

53 ure MCD spectra reveal significant shifts in electronic transition energies that are correlated to di

54 te zero-field splitting (ZFS) parameters and electronic transition energies, intensities, and polariz

55 ne ground-state spin Hamiltonian parameters, electronic transition energies, oscillator strengths, an

56 mall despite large changes in the calculated electronic transition energies.

57 l, and acetonitrile cause blue shifts in the electronic transition energy of the bare m-nitrophenolat

58 The electronic transitions for solid Mo(4)PFT (lowest at 410

59 structural lattice distortion followed by an electronic transition from a semiconducting to metallic

60 density toward the cation with a subsequent electronic transition from the HOMO-2 to the HOMO.

61 ctors for the lowest energy molecular nature electronic transition have been calculated and the origi

62 so reproduces the switching of the nature of electronic transition in higher homologues of (R2N)PPn(+

63 eity but identified a new, to our knowledge, electronic transition in the absorption profile at 644 n

64 We investigate the assignment of electronic transitions in alkyl peroxy radicals.

65 based magnetometer, employing spin-dependent electronic transitions in an organic diode, which combin

66 Electronic transitions in aromatic side chains are respo

67 There is a great interest in electronic transitions in hydrogen-rich materials under

68 ence weak spin-orbit interaction can control electronic transitions in molecular and solid-state syst

69 applications, including the spectroscopy of electronic transitions in molecules, experimental tests

70 tuning the energy difference between the two electronic transitions in the dimer to match a vibration

71 es of radical ligands can exhibit low-energy electronic transitions in the near-infrared (NIR) spectr

72 Urocanic acid, UCA, is characterized by two electronic transitions in the UV-B (280-320 nm) which co

73 he W-L complexes, to simulate and assign the electronic transitions in the UV-vis spectra, to determi

74 tion symmetries display absorptive 4f --> 5d electronic transitions in the visible region.

75 ng potential, permitting coherent control of electronic transitions independent of the atomic center-

76 ltimate efficiencies by the type of emissive electronic transitions involved.

77 esponse theory allowed identification of the electronic transitions involved.

78 ethyl-THF glass) in the UV-vis region to (1) electronic transitions involving the four-center orbital

79 f the excited state is a triplet because the electronic transition is 'dark' with a vanishing oscilla

80 This electronic transition is accompanied by a dramatic struc

81 The electronic transition is attributed to the electric-fiel

82 A high-frequency (3300-2600 cm(-1)) electronic transition is observed for all PS I particles

83 e existence of a universal alignment for the electronic transition level of hydrogen in semiconductor

84 ctroelectrochemical data with the calculated electronic transitions makes it possible to both evidenc

85 Electronic transition moments and circular dichroism ten

86 behaviour originates from the suppression of electronic transitions near the Weyl points due to the d

87 upling between an infrared-active phonon and electronic transitions near the Weyl points through the

88 The most bathochromic electronic transition of the chromophores essentially ex

89 The low-energy electronic transition of the PP(2)-PP(7) cation radicals

90 rmed to analyze the orbitals involved in the electronic transitions of 4, 6, and 7.

91 ientations and intensities of the low-energy electronic transitions of 6-MI reported here should be u

92 or a particular size n, the measured valence electronic transitions of all these systems fall into ei

93 deration of the vibrational structure of the electronic transitions of aromatic side chains.

94 bility to tune the emission is attributed to electronic transitions of mixed ligand-to-metal-metal-ch

95 arise from circular dichroism of the strong electronic transitions of photosynthetic absorption band

96 rational spectra and TDDFT simulation of the electronic transitions of potential photointermediates c

97 Furthermore, the electronic transitions of R6G on Ag surface were studied

98 The electronic transitions of several -C(5)- carbenes are co

99 The d-d electronic transitions of the Co(II)-substituted hexamer

100 The major electronic transitions of the light-harvesting complex o

101 oupling in an optical microcavity to mix the electronic transitions of two J-aggregated molecular dye

102 vis region of the spectra are due to pi-pi* electronic transitions, of an intramolecular charge-tran

103 nesiowustite and the isolated effects of the electronic transitions on the elasticity of magnesiowust

104 rescent ligands to be probed even when their electronic transitions overlap with those of the macromo

105 -positions of the macrocycles results in new electronic transitions polarized along the long axes of

106 e further insight into the energy levels and electronic transitions present, computational studies of

107 s been analyzed to obtain information on the electronic transitions responsible for the linkage isome

108 t probably related to the two-photon allowed electronic transition S0-->S2.

109 at 50-1400 cm(-1) , which was attributed to electronic transitions, scattering, photoluminescent emi

110 In addition, the electronic transition state of graphene within the UV re

111 or studying elusive quantum effects in which electronic transitions strongly couple to phonons and vi

112 dicate that these divide into three types of electronic transitions; t(2) --> t(2) involving excitati

113 in the UV spectral region where the relevant electronic transitions take place, we have developed and

114 The accessible electronic transitions, term energies, and orbital angul

115 r UV-absorption spectra show a lowest energy electronic transition that decreases in energy (3.54 eV,

116 ength (457 nanometers) in the vicinity of an electronic transition that shows circular dichroism in b

117 , which is accomplished by targeting special electronic transitions that allows for a fast screening

118 understanding of the metal-metal bonding and electronic transitions that are responsible for their UV

119 line width is a result of multiple, discrete electronic transitions that couple to vibrations of the

120 tum chemical calculations, we identified six electronic transitions that occur within the 25,000-50,0

121 uires that the dipole moment of the resonant electronic transition, the change of the dipole moment u

122 ficant density change is observed across the electronic transition, the jump in the sound velocities

123 eting electronic states; it is thus a purely electronic transition to a superconducting state, with a

124 by coupling photons generated from interband electronic transition to phonon polariton modes on the s

125 ld enables us to control and manipulate this electronic transition to the extent that a p-n junction

126 nd within the aromatic amino acid pi --> pi* electronic transitions to examine the temperature depend

127 ed species also shifts the near-IR interband electronic transitions to lower energy by more than 10%.

128 e apply a new algorithm for modeling protein electronic transitions to simulate two-dimensional UV ph

129 phenol, and indole that describe the valence electronic transitions to the (1)L(b), (1)L(a), (1)B(b),

130 With consumer electronics transitioning toward flexible products, ther

131 candidate for inducing coupled magnetic and electronic transition via fast and reversible redox reac

132 conductor with light that resonates with its electronic transition, we find that halide-containing ar

133 h-spin diiron(II) complexes with distinctive electronic transitions were prepared by using 4-cyanopyr

134 e the bound dyes (with calf thymus DNA) have electronic transitions with lambda(max) = 514 nm (comple

135 ansition of the ABC-flavanone moiety and the electronic transition within the DEF-flavone moiety, whi

136 y and the DEF-flavone moiety, as well as the electronic transition within the DEF-flavone moiety.